755 - 764 |
Granulation and bistability in non-Brownian suspensions Cates ME, Wyart M |
765 - 777 |
Scaling relations for elongational flow of polystyrene melts and concentrated solutions of polystyrene in oligomeric styrene Wagner MH |
779 - 790 |
Rheological and foaming behavior of linear and branched polylactides Najafi N, Heuzey MC, Carreau PJ, Therriault D, Park CB |
791 - 804 |
Numerical study of the combined effects of inertia, slip, and compressibility in extrusion of yield stress fluids Kountouriotis Z, Georgiou GC, Mitsoulis E |
805 - 815 |
Physical characterisation and yield stress of a concentrated Miscanthus suspension Botto L, Preuss K, Robertson LX, Xu XY |
817 - 829 |
Predicting extrusion instabilities of commercial polyethylene from non-linear rheology measurements Cyriac F, Covas JA, Hilliou LHG, Vittorias I |
831 - 841 |
A model for the shear viscosity of non-colloidal suspensions with Newtonian matrix fluids Housiadas KD, Tanner RI |
843 - 855 |
Observations on the rheological response of alkali activated fly ash suspensions: the role of activator type and concentration Vance K, Dakhane A, Sant G, Neithalath N |
857 - 868 |
Phase behavior and effects of microstructure on viscoelastic properties of a series of polylactides and polylactide/poly(epsilon-caprolactone) copolymers Ugartemendia JM, Munoz ME, Sarasua JR, Santamaria A |
869 - 882 |
A rheological criterion to determine the percolation threshold in polymer nano-composites Hassanabadi HM, Wilhelm M, Rodrigue D |